Research Article Volume 8 Issue 2
National Research University of Electronic Technology, Russia
Correspondence: Afonin SM, National Research University of Electronic Technology MIET, Moscow, Russia
Received: June 20, 2024 | Published: July 2, 2024
Citation: Afonin SM. Frequency method for determination self-oscillations in control systems with a piezo actuator for astrophysical research. Aeron Aero Open Access J. 2024;8(2):115-117. DOI: 10.15406/aaoaj.2024.08.00198
For the control system with a piezo actuator in astrophysical research the condition for the existence of self-oscillations is determined. Frequency method for determination self-oscillations in control systems is applied. By using the harmonious linearization of hysteresis and Nyquist stability criterion the condition of the existence of self-oscillations is obtained.
Keywords: frequency method, control system, piezoactuator, hysteresis, self-oscillations, astrophysical research
A piezo actuator is used in astrophysics for image stabilization and scan system.1–19 Frequency method for determination self-oscillations in scan system is applied.20–46 for Nyquist stability criterion of self-oscillations at harmonious linearization of hysteresis characteristic of a piezo actuator.
Condition of self-oscillations
The scan system with a piezo actuator is used for astrophysical research in system adaptive optics. Nyquist stability criterion of self-oscillations at harmonious linearization of hysteresis characteristic2,20–40 of a piezo actuator has the form
Wl(αΩ) Wg(Em max)=−1Wl(αΩ)Wg(Emmax)=−1
where α is the imaginary unit, Ω - the frequency of self-oscillations, Wl(αΩ)Wl(αΩ) - the frequency transfer function of the linear part, Wg(Em max)Wg(Emmax) - the transfer function of the hysteresis part, Em maxEmmax - amplitude of the electric field strength for m axis.
For the scan system with a piezo actuator for astrophysical research the condition of self-oscillations is written
1+Wl(αΩ) Wg(Em max)=01+Wl(αΩ)Wg(Emmax)=0
The condition of self-oscillations is determined in the form
Wl(αΩ)=−1Wg(Em max)Wl(αΩ)=−1Wg(Emmax)
here the left side of this equation has the form of the amplitude-phase characteristic of the linear part of the system, and the right side of the equation has the form of the inverse amplitude-phase characteristic of the hysteresis link of the piezo actuator with the inverse sign minus.
Preisach hysteresis function a piezo actuator has the form22-40
Si=F[Em|t0,t,Si(0),sign˙Em]Si=F[Em|t0,t,Si(0),sign˙Em]
here t,Si,Si(0),Emt,Si,Si(0),Em and sign˙Emsign˙Em - the time, the deformation, the initial deformation,, the strength of electric field and the sign velocity.
The symmetric hysteresis the deformation22-40 a piezo actuator has the form
Si=dmiEm−γmiEm max(1−E2mE2m max)nsign˙EmSi=dmiEm−γmiEmmax(1−E2mE2mmax)nsign˙Em
dmi=d0mi+amiE2m,γmi=S0i/Em maxdmi=d0mi+amiE2m,γmi=S0i/Emmax
here dmi,γmi,S0i,ndmi,γmi,S0i,n , - the piezo module, the hysteresis coefficient, the relative deformation for Em=0Em=0 , and the power 1, 2, 3, ….
The transfer function of the linear part of the scan system with a piezo actuator for elastic-inertia load22,37-46 has the form
Wl(p)=klT2tp2+2Ttξtp+1Wl(p)=klT2tp2+2Ttξtp+1
After transformations we have this condition for the scan system with the PZT actuator at the power in the form
11−T2tΩ2kl+α2TtξtΩkl=1− (d0mi+amiE2m max)+α8γmi3π11−T2tΩ2kl+α2TtξtΩkl=1−(d0mi+amiE2mmax)+α8γmi3π
Ω=4γmikl3πTtξt
For the the scan system with the PZT actuator = 3.2×108 V/m, d033 = 4×10-10 m/V, γ33 = 0.8×10-10 m/V, a33 = 3.1×10-22 m3/V3, Tt = 10-3 s, ξt = 10-2 the frequency is determined Ω =1.1×103 s-1 with error of 10 %.
The frequency transfer function of the symmetric hysteresis the deformation of a piezo actuator is received in the form
Wg(Em max)=Si(Em max)/Em(Em max)
Wg(Em max)=qmi(Em max)+αq′mi(Em max)
For n = 1
qmi(Em max)=dmi,q′mi(Em max)=− 4⋅2⋅γmiπ⋅3=− 8γmi3π
For n = 2
qmi(Em max)=dmi,q′mi(Em max)=− 4⋅2⋅4⋅γmiπ⋅3⋅5=− 32γmi15π
For n = 2
qmi(Em max)=dmi,q′mi(Em max)=− 4⋅2⋅4⋅6⋅γmiπ⋅3⋅5⋅7=− 192γmi105π
For n to n + 1
qmi(Em max)=dmi,q′mi(n)(Em max)=2n2n+1q′mi(n−1)(Em max)
For n + 1
qmi(Em max)=dmi,q′mi(Em max)=− 4⋅2⋅4⋅6⋅...⋅2n⋅γmiπ⋅3⋅5⋅7⋅...⋅(2n+1)
The stability criterion and frequency method are used.
By using of frequency method the parameters of self-oscillations are obtained in the scan system. Nyquist stability criterion is used for calculation the self-oscillations in the control system with a piezo actuator at harmonious linearization of hysteresis characteristic of a piezo actuator.
For the scan system its condition of self-oscillations is determined. For calculation the self-oscillations frequency method is applied at harmonious linearization of hysteresis characteristic of a piezo actuator.
None.
The authors declare that there is no conflict of interest.
©2024 Afonin. This is an open access article distributed under the terms of the, which permits unrestricted use, distribution, and build upon your work non-commercially.